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arXiv 2608.00688astro-ph.GAastro-ph.SR

恒星级黑洞对河外H II区的光谱微引力透镜

Spectral Microlensing of Extragalactic H II Regions by Stellar-Mass Black Holes

Dezi Liu

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中文总结 AI 辅助

该研究提出通过恒星级黑洞对河外致密H II区的光谱微引力透镜效应,探测银晕等区域的孤立恒星级黑洞,为约束其丰度提供了新途径。

中文摘要 AI 辅助

银河系中大部分预测存在的恒星级黑洞仍未被探测到,尤其是在银极高纬度区域或银晕中,传统的密场恒星星微引力透镜方法在此类区域无效。我们提出一种替代方法,通过对致密河外H II区的光谱微引力透镜来绘制这一孤立黑洞种群的分布。在源平面上,银河系黑洞的物理爱因斯坦半径可与遥远星系中H II区的典型核心尺寸匹配。微引力透镜会触发消色差放大,在积分星系光谱中产生独特的窄发射线过剩。由于引力透镜与波长无关,固有线比率得以保留,这为区分假阳性天体物理瞬变事件提供了可靠依据。值得注意的是,该方法的效率关键取决于H II区的尺寸:延展区域的光学深度较低,而物理尺寸≤10 pc的致密核心可提供显著更高的放大率。不过这些致密核心在光学波长上受尘埃严重遮挡,因此红外和射电观测是该方法的主要观测窗口。即便如此,背景H II区的空间稀疏性以及高放大率所需的严格对准要求,使得预期的事件率限制为每年约10⁻⁶。尽管如此,该方法提供了一个独特的机会,可探测恒星级黑洞并约束其在这类低密度环境中的丰度。

英文摘要

Most of the Milky Way's predicted stellar-mass black holes remain hidden, especially at high Galactic latitudes or in the Galactic halo, where traditional dense-field stellar microlensing is ineffective. We propose an alternative method to map this isolated population via the spectral microlensing of compact, extragalactic H II regions. Projected onto the source plane, the physical Einstein radius of a Galactic black hole can match the typical core sizes of H II regions in distant galaxies. Microlensing triggers an achromatic magnification, producing distinct narrow emission-line excesses in integrated galaxy spectra. Because gravitational lensing is wavelength-independent, intrinsic line ratios are preserved, offering a robust discriminant against false-positive astrophysical transients. Notably, the efficiency of this method depends critically on the size of the H II regions: while extended regions suffer from low optical depth, compact regions with a physical size $\lesssim 10$ pc offer significantly higher magnifications. These compact cores, however, are heavily dust-obscured at optical wavelengths, making infrared and radio observations the primary windows for this method. Even so, the spatial sparseness of background H II regions and the stringent alignment requirement for high magnification limit the expected event rate to $\sim 10^{-6}$ per year. Nevertheless, this method offers a unique opportunity to detect stellar-mass black holes and constrain their abundance in such low-density environments.

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